b
(b) According to question resistance of wire $ADC$ is twice that of wire $ABC$. Hence current flows through $ADC$ is half that of $ABC$ i.e. $\frac{{{i_2}}}{{{i_1}}} = \frac{1}{2}$. Also ${i_1} + {i_2} = i$ $==>$ ${i_1} = \frac{{2i}}{3}$ and ${i_2} = \frac{i}{3}$
Magnetic field at centre $O$ due to wire $AB$ and $BC$ (part $1$ and $2$) ${B_1} = {B_2} = \frac{{{\mu _0}}}{{4\pi }}.\frac{{2{i_1}\sin {{45}^o}}}{{a/2}} \otimes $$ = \frac{{{\mu _0}}}{{4\pi }}.\frac{{2\sqrt 2 \,{i_1}}}{a} \otimes $
and magnetic field at centre $O$ due to wires $AD$ and $DC$ (i.e. part $3$ and $4$) ${B_3} = {B_4} = \frac{{{\mu _0}}}{{4\pi }}\frac{{2\sqrt 2 \,{i_2}}}{a}\odot$
Also $i_1 = 2i_2. \,So \,(B_1 = B_2) > (B_3 = B_4)$
Hence net magnetic field at centre $O$
${B_{net}} = ({B_1} + {B_2}) - ({B_3} + {B_4})$
$ = 2 \times \frac{{{\mu _0}}}{{4\pi }}.\frac{{2\sqrt 2 \, \times \left( {\frac{2}{3}i} \right)}}{a} - \frac{{{\mu _0}}}{{4\pi }}.\frac{{2\sqrt 2 \,\left( {\frac{i}{3}} \right) \times 2}}{a}$
$ = \frac{{{\mu _0}}}{{4\pi }}.\frac{{4\sqrt 2 \,i}}{{3a}}(2 - 1)\, \otimes = \frac{{\sqrt 2 \,{\mu _0}i}}{{3\pi \,a}} \otimes $